Towards the discovery of new physics with lepton-universality ratios of b →sℓℓ decays

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Abstract

Tests of lepton-universality as rate ratios in b→sℓℓ transitions can be predicted very accurately in the Standard Model. The deficits with respect to expectations reported by the LHCb experiment in muon-To-electron ratios of the B→K(∗)ℓℓ decay rates thus point to genuine manifestations of lepton nonuniversal new physics. In this paper, we analyze these measurements in the context of effective field theory. First, we discuss the interplay of the different operators in RK and RK∗ and provide predictions for RK∗ in the Standard Model and in new-physics scenarios that can explain RK. We also provide approximate numerical formulas for these observables in bins of interest as functions of the relevant Wilson coefficients. Secondly, we perform frequentist fits to RK and RK∗. The Standard Model disagrees with these measurements at 3.7σ significance. We find excellent fits in scenarios with combinations of O9(10)ℓ=s γμbLℓγμ(γ5)ℓ operators, with pulls relative to the Standard Model in the region of 4σ. An important conclusion of our analysis is that a lepton-specific contribution to O10 is important to understand the data. Under the hypothesis that new-physics couples selectively to the muons, we also present fits to other b→sμμ data with a conservative error assessment and comment on more general scenarios. Finally, we discuss new lepton universality ratios that, if new physics is the origin of the observed discrepancy, should contribute to the statistically significant discovery of new physics in the near future.

Figures

  • FIG. 1. RK and RK (in the ½1.1; 6 GeV2 bin) parametric dependence on one Wilson coefficient at a time, for NP affecting only the muonic coefficients, where the nodes indicate steps of ΔðδCμÞ ¼ þ0.5 from the SM point and in the direction of the arrows. The red solid line shows the dependence on δCμ9, dashed blue line on δCμ10, green dot-dashed on δC 0μ 9 and orange dotted on δC0μ10.
  • FIG. 2. Results for RK and RK in the SM and various NP scenarios as a function of the invariant mass of the lepton pair, q2. Solid gray line corresponds to the SM, solid red line to the scenario in which δCμ9 ¼ −1, dot-dashed orange line to δCμ10 ¼ 1, dashed green line to δC0μ9 ¼ −1 and blue dotted line to δCμL ¼ −0.5. The shadings around each curve indicates our estimate of the hadronic uncertainties (see main text). We overlay the experimental LHCb results shown in black as points with error bars.
  • TABLE I. Results for binned observables in the SM and different NP scenarios using the approach described in Ref. [29]. The errors are obtained with the Gaussian method described in Ref. [29] for the distributions of the hadronic parameters. The experimental results have been rounded conservatively by taking the larger side of the statistical error and adding the systematic in quadrature, and neglecting correlations. We show also predictions for the high q2 bin.
  • FIG. 3. The top panel shows the result of a fit to a model that includes muon-specific NP Wilson coefficients δCμ9 and δC μ 10. The cross indicates the position of the minimum. The first two graphs in the bottom row give the χ2 distribution projected onto each Wilson coefficient, while the third one is projected onto the difference δCμL ¼ δCμ9 − δCμ10. Ranges in orange and light red correspond to 1 and 3σ intervals of Wilson coefficients, respectively. [Δχ2 ¼ 1ð9Þ for 1σð3σÞ in the 1-parameter cases, Δχ2 ¼ 2.3ð11.83Þ for 1σð3σÞ in the 2-parameter fit.]
  • TABLE II. Best fit values, goodness of fit, p-value, SM exclusion level (pull), and confidence intervals for fits of single or pairs of Wilson coefficients, to RK and RK data. For the one-dimensional case, we show the 1σ and 3σ confidence intervals, while for the two-dimensional case we show the 1σ intervals for the two parameters instead.
  • TABLE III. As in Table II but in fits to RK , RK and Bs → μμ data.
  • FIG. 4. Contours at 1σ and 3σ level in the ðδCμ9; δCμ10Þ plane, in solid lines and orange and light-red colors, for the fit to RK , RK and BRðBs → μμÞ. We also show the 1σ and 3σ constraints given individually by RK, RK in the ½1.1; 6 GeV2 bin and BRðBs → μμÞ using blue, green and gray contours, respectively. The cross indicates the position of the minimum.
  • TABLE IV. Same as Table III, but with BRðB → K γÞ, the B → K μμ angular distribution and Qi observables added to the data set.

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Geng, L. S., Grinstein, B., Jäger, S., Martin Camalich, J., Ren, X. L., & Shi, R. X. (2017). Towards the discovery of new physics with lepton-universality ratios of b →sℓℓ decays. Physical Review D, 96(9). https://doi.org/10.1103/PhysRevD.96.093006

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